Solving the Boat Crossing a River Problem using the Calculus of Variations

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Discussion Overview

The discussion revolves around the application of the Calculus of Variations to solve the problem of determining the minimum time for a boat to cross a river, particularly focusing on the conditions under which the path taken is a straight line. Participants explore both the theoretical aspects of the problem and its practical implications, including a related scenario involving a lifeguard reaching a swimmer.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant seeks to prove that the minimum time for crossing the river results in a straight-line path, using equations of motion and the Calculus of Variations.
  • Another participant argues that the straight-line path is evident due to zero acceleration, suggesting that using the Calculus of Variations may be excessive for this problem.
  • A different participant introduces an analogous problem involving a lifeguard, questioning whether the original problem requires the Calculus of Variations or if it can be solved through standard optimization methods.
  • Some participants discuss the merits of using the Calculus of Variations for simple examples, asserting that it can effectively demonstrate fundamental concepts.
  • There is a suggestion to explore both standard optimization techniques and the Calculus of Variations to find the shortest time for the lifeguard to reach the swimmer.
  • Participants express uncertainty about the complexity of the mathematical expressions involved in the optimization process and the potential for simplification.
  • One participant emphasizes the importance of finding conditions that minimize time by varying the path and analyzing the limit as the variation approaches zero.

Areas of Agreement / Disagreement

Participants do not reach a consensus on whether the Calculus of Variations is necessary for solving the original problem, with some advocating for its use while others suggest simpler methods may suffice. The discussion remains unresolved regarding the best approach to take.

Contextual Notes

Participants express varying levels of familiarity with the Calculus of Variations, leading to different interpretations of its application. There are also unresolved mathematical steps and assumptions regarding the conditions for minimizing time in both the original and analogous problems.

Who May Find This Useful

This discussion may be of interest to students and practitioners in physics and mathematics, particularly those exploring optimization problems and the Calculus of Variations in practical scenarios.

  • #31
Now can we talk about how this works?

Choose an optimum set of paths ( for this problem ), and deviate from it by some amount ## \delta##.

For this problem we demanded the total deviation from optimum be zero.

Firstly, how is that possible? I would think we should not be able to deviate at all from an optimum path with no net change in the optimized parameter.

Secondly, what happens if there is no optimum path. i.e. we try to optimize something that is not optimizable with this technique? It seems like we should have to have prior knowledge about the existence of an optimum before this can be applied?
 
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  • #32
malawi_glenn said:
Works for me. But one might have to hit refresh on the browser now and then
Thats right, if there is latex in the thread this will work. I forgot.
 
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  • #33
These are good questions.
erobz said:
Now can we talk about how this works?

Choose an optimum set of paths ( for this problem ), and deviate from it by some amount ## \delta##.
That's not what I wrote in item 1, post #12. There is only one optimum path and you start by assuming that you have found it. You give a placeholder name to a parameter that specifies it and the task is to find the value of this placeholder parameter in terms of the given quantities.
erobz said:
Firstly, how is that possible? I would think we should not be able to deviate at all from an optimum path with no net change in the optimized parameter.
You can calculate times for any path for a choice of ##\delta##. If two different values of ##\delta## give the same time, then neither of the two paths can be optimum. However, the optimum should be between the two values of ##\delta##, one of which must be positive and the other negative. Do you see why?
erobz said:
Secondly, what happens if there is no optimum path. i.e. we try to optimize something that is not optimizable with this technique? It seems like we should have to have prior knowledge about the existence of an optimum before this can be applied?
You cannot find something that doesn't exist. That is why before starting out to optimize a function, you need to ascertain that it can be optimized. That is what I did in post #22 when I argued that the optimum path must be at a crossing point situated between points C and D.
 
  • #34
kuruman said:
You can calculate times for any path for a choice of ##\delta##. If two different values of ##\delta## give the same time, then neither of the two paths can be optimum. However, the optimum should be between the two values of ##\delta##, one of which must be positive and the other negative. Do you see why?

Well, I think because we've chosen the coordinate ##x ## to be at an extremum, that is either concave up ( local minimum ) or concave down ( local maximum ) in the vicinity of ##x##. So I agree that the change in time could be zero with ##\pm \delta##.

You emphasized that we deviate a small amount ## \delta ##. What is the significance of that in this context?

I see that ##\delta \ll x## is significant, because it can't become small arbitrarily small or else, we get ## 0 + 0 = 0 ##. This Is like a linearization in that way around ##x##.
 
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